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Merge branch 'master' of github.com:moorepants/learn-multibody-dynamics
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@@ -195,6 +195,11 @@ then:
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= \bar{F}
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\in \mathbb{R}^{6\nu}
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.. note:: If the measure numbers are instead extracted from the dyadics and
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vectors expressed in the associated rigid bodies' reference frames,
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:math:`\mathbf{M}` is constant with respect to time and thus
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:math:`\dot{\mathbf{M}} = 0`.
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Subsituting the mapping to generalized speeds :math:`\dot{\bar{v}} =
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\dot{\mathbf{T}} \bar{u} + \mathbf{T} \dot{\bar{u}}` gives:
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